E. S. Smith
Thomas Jefferson National Accelerator Facility
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Featured researches published by E. S. Smith.
Physical Review Letters | 2013
Bulatowicz M; Griffith R; Michael Larsen; Mirijanian J; Fu Cb; E. S. Smith; W. M. Snow; Yan H; Thad G. Walker
Various theories beyond the standard model predict new particles with masses in the sub-eV range with very weak couplings to ordinary matter. A new P-odd and T-odd interaction between polarized and unpolarized nucleons proportional to K·r is one such possibility, where r is the distance between the nucleons and K is the spin of the polarized nucleon. Such an interaction involving a scalar coupling gs at one vertex and a pseudoscalar coupling gp at the polarized nucleon vertex can be induced by the exchange of spin-0 bosons. We used the NMR cell test station at Northrop Grumman Corporation to search for NMR frequency shifts in polarized 129Xe and 131Xe when a nonmagnetic zirconia rod is moved near the NMR cell. Long (T2∼20 s) spin-relaxation times allow precision measurements of the NMR frequency ratios, which are insensitive to magnetic field fluctuations. Combined with existing theoretical calculations of the neutron spin contribution to the nuclear angular momentum in xenon nuclei, the measurements improve the laboratory upper bound on the product gsgp(n) by 2 orders of magnitude for distances near 1 mm. The sensitivity of this technique can be increased by at least two more orders of magnitude.
Physical Review D | 2013
Pinghan Chu; Alec Dennis; Changbo Fu; H. Gao; Rakshya Khatiwada; G. Laskaris; Ke Li; E. S. Smith; William Snow; Haiyang Yan; W. Zheng
The possible existence of short-range forces between unpolarized and polarized spin-1/2 particles has attracted the attention of physicists for decades. These forces are predicted in various theories and provide a possible new source for parity (P) and time reversal (T) symmetry violation. We use an ensemble of polarized 3He gas in a cell with a 250 um thickness glass window to search for a force from scalar boson exchange over a sub-millimeter ranges. This interaction would produce a NMR frequency shift as an unpolarized mass is moved near and far from the polarized ensemble. We report a new upper bound on the product g_{s}g_{p}^{n} of the scalar couplings to the fermions in the unpolarized mass, and the pseudoscalar coupling of the polarized neutron in the 3He nucleus for force ranges from 1e-4 to 1e-2 m, which corresponds to a mass range of 2e-3 to 2e-5 eV for the scalar boson.
Communications in Computational Physics | 2014
Haiyang Yan; Ke Li; Rakshya Khatiwada; E. S. Smith; W. M. Snow; Changbo Fu; Pinghan Chu; H. Gao; W. Zheng
We present a high precision frequency determination method for digitized NMR FID signals. The method employs high precision numerical integration rather than simple summation as in many other techniques. With no independent knowledge of the other parameters of a NMR FID signal (phase
arXiv: Instrumentation and Detectors | 2017
M. Battaglieri; F. X. Girod; A. Murphy; R. De Leo; G. Simi; M. Taiuti; K. Hicks; M. De Napoli; R. Peremuzyan; Gordan Krnjaic; C. Sutera; L. Lagamba; G. Russo; I. Zonta; E. Leonora; S. Anefalos Pereira; B. McKinnon; V. Lucherini; M. Carpinelli; A. D'Angelo; Philip Schuster; D. Sokhan A. Afanasev; F. Spizzo; E. Santopinto; N. Randazzo; M. Ungaro; M. Holtrop; E. Cisbani; Natalia Toro; M. Sperduto
\phi
arXiv: Nuclear Experiment | 2013
Aleksandrs Aleksejevs; R. White; Y. Qiang; W. I. Levine; F. Close; E. Chudakov; T. Whitlatch; G. J. Lolos; V. Crede; I. Senderovich; N. Jarvis; J. Leckey; P. Mattione; S.T. Krueger; Eric S. Swanson; A. Ponosov; Adam P. Szczepaniak; M.J. Staib; P. Collins; A. Somov; P. Khetarpal; P. Eugenio; O. Soto; R. A. Schumacher; D. Lawrence; F. Klein; S. Somov; E. Wolin; J. Hardin; S. Taylor
, amplitude
arXiv: High Energy Physics - Experiment | 2012
M. Dugger; P. Eugenio; Jozef J. Dudek; R. A. Schumacher; D. Lawrence; F. Klein; D. Bennett; H. Egiyan; B. G. Ritchie; Günter Huber; M. M. Ito; W. K. Brooks; E. Pooser; P. Ioannou; L. Pentchev; L. Gan; A. Barnes; F. Close; C. Kourkoumeli; M. Tahani; D. I. Sober; J. Bennett; P. Ambrozewicz; L. Guo; H. Al Ghoul; J. Leckey; N. Sparks; A. Semenov; F. Barbosa; G. J. Lolos
A
Physics Letters B | 2012
L. Guo; C. Hanretty; K. Hicks; R. J. Holt; C. E. Hyde; Y. Ilieva; D. G. Ireland; B. S. Ishkhanov; E. L. Isupov; S. S. Jawalker; D. Keller; M. Khandaker; P. Kheterpal; A. Kim; W. Kim; A. Klein; F. J. Klein; V. Kubarovsky; S. E. Kuhn; S. Kuleshov; V. Kuznetsov; J. M. Laget; H. Y. Lu; I. D. J. MacGregor; Y. Mao; N. Markov; M. Mayer; J. McAndrew; B. McKinnon; C. Meyer
, and transverse relaxation time
Physical Review C | 2012
M. Anghinolfi; J. Ball; N. A. Baltzell; M. Battaglieri; I. Bedlinskiy; M. Bellis; A. S. Biselli; C. Bookwalter; S. Boiarinov; P. Bosted; V. D. Burkert; D. S. Carman; A. Celentano; S. Chandavar; P. L. Cole; V. Crede; R. De Vita; E. De Sanctis; B. Dey; R. Dickson; D. Doughty; M. Dugger; R. Dupre; H. Egiyan; A. El Alaoui; L. El Fassi; L. Elouadrhiri; P. Eugenio; G. Fedotov; M. Y. Gabrielyan
T_{2}
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2018
T.D. Beattie; A.M. Foda; C.L. Henschel; S. Katsaganis; S.T. Krueger; G. J. Lolos; Z. Papandreou; E.L. Plummer; I.A. Semenova; A. Yu Semenov; F. Barbosa; E. Chudakov; M.M. Dalton; D. Lawrence; Y. Qiang; N. Sandoval; E. S. Smith; C. Stanislav; J. R. Stevens; S. Taylor; T. Whitlatch; B. Zihlmann; W. I. Levine; W. McGinley; C. Meyer; M.J. Staib; E. Anassontzis; C. Kourkoumelis; G. Vasileiadis; G. Voulgaris
) this method can determine the signal frequency
Bulletin of the American Physical Society | 2015
E. S. Smith
f_{0}